We study theoretically a novel Bardeen-Cooper-Schrieffer (BCS) to Bose-Einstein condensate (BEC) crossover of two-specie ions in a three-dimensional quantum plasma at zero temperature. Central to this crossover is an effective short-ranged, attractive interaction potential between the ions shielded by the surrounding degenerate electrons. The interaction range and magnitude can be tuned non-monotonically by varying the carrier density of the quantum plasma. Low-energy collisions between two ions are characterized by the s-wave scattering length when the interaction range and the inter-ion spacing are comparable. We show that the s-wave scattering length can be changed from −∞ to ∞, leading to a BCS-BEC crossover driven purely by the plasma density. Through numerical and analytical calculations, we find that the quantum acoustic waves in the plasma exhibit distinct dispersion relations in the different regimes, providing a route to probe the crossover. Our study shows that the quantum plasma may offer a new platform to quantum simulate the BEC-BCS crossover and exotic phases with added tunability that might be difficult to achieve in conventional solid-state systems and ultracold atom gases.